The mathematics of classical mechanics Newton’s Laws of motion: 1) inertia 2) F = ma 3) action:reaction The motion of particle is represented as a differential.

Slides:



Advertisements
Similar presentations
Ch. 13 Electrons in Atoms Ch Models of the Atom
Advertisements

Wave-Particle Duality
7-1 Dr. Wolf’s CHM 101 Chapter 7 Quantum Theory and Atomic Structure.
Ch 9 pages ; Lecture 20 – Particle and Waves.
The photoelectric effect and the photon theory of light
Black body radiation BBR is the radiation emitted by a non-reflecting solid body. A perfect black body is one which absorbs all the radiations falling.
1 Light as a Particle The photoelectric effect. In 1888, Heinrich Hertz discovered that electrons could be ejected from a sample by shining light on it.
PHY 102: Quantum Physics Topic 3 De Broglie Waves.
Electromagnetic Radiation
The Electronic Structures of Atoms Electromagnetic Radiation
Arrangement of Electrons in Atoms The Development of a New Atomic Model.
Atomic Theories Democritus (300 B. C.)
Pre-IB/Pre-AP CHEMISTRY
Electronic Structure of Atoms
Properties of Light Is Light a Wave or a Particle?
Physics at the end of XIX Century Major Discoveries of XX Century
Vacuum tube - V, only for shorter than certain wavelength Current V VoVo Fixed wavelength Varying intensity I2I 3I Maximum electron energy 0.
Classical vs Quantum Mechanics Rutherford’s model of the atom: electrons orbiting around a dense, massive positive nucleus Expected to be able to use classical.
The Photoelectric Effect
Quantum Physics. Black Body Radiation Intensity of blackbody radiation Classical Rayleigh-Jeans law for radiation emission Planck’s expression h =
Chapter 71 Atomic Structure Chapter 7. 2 Electromagnetic Radiation -Visible light is a small portion of the electromagnetic spectrum.
Early Quantum Theory and Models of the Atom
Quantum Theory of the Atom
Physics 1C Lecture 29A.
Modern Physics.
Electronic Structure of Atoms Chapter 6 BLB 12 th.
1 Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Quantum Theory and the Electronic Structure of.
Particle Nature of Light
Chapter 39 Particles Behaving as Waves
ELECTRONICS II VLSI DESIGN FALL 2013 LECTURE 1 INSTRUCTOR: L.M. HEAD, PhD ELECTRICAL & COMPUTER ENGINEERING ROWAN UNIVERSITY.
Chapter 10: Modern atomic theory Chemistry 1020: Interpretive chemistry Andy Aspaas, Instructor.
Chapter 6: Electronic Structure of Atoms Pages
Early Quantum Theory AP Physics Chapter 27. Early Quantum Theory 27.1 Discovery and Properties of the Electron.
Quantum Mechanics. Planck’s Law A blackbody is a hypothetical body which absorbs radiation perfectly for every wave length. The radiation law of Rayleigh-Jeans.
Quantum Physics. Quantum Theory Max Planck, examining heat radiation (ir light) proposes energy is quantized, or occurring in discrete small packets with.
Quantum Theory and the Electronic Structure of Atoms Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Leading up to the Quantum Theory.  exhibits wavelike behavior  moves at a speed 3.8 × 10 8 m/s in a vacuum  there are measureable properties of light.
Chemistry is in the electrons Electronic structure – how the electrons are arranged inside the atom Two parameters: –Energy –Position.
Chemistry 330 Chapter 11 Quantum Mechanics – The Concepts.
Chapter 27- Atomic/Quantum Physics
What’s coming up??? Oct 25The atmosphere, part 1Ch. 8 Oct 27Midterm … No lecture Oct 29The atmosphere, part 2Ch. 8 Nov 1Light, blackbodies, BohrCh. 9 Nov.
Chapter 2 Intro to quantum mechanics. Why do we need QM?  Classical physics is great for large objects, but fails when it comes to atomic particles like.
Quantum Theory Waves Behave Like Particles Maxwell’s Wave Theory (1860) Maxwell postulated that changing electric fields produce changing magnetic fields:
Classical Physics Newton’s laws: Newton’s laws: allow prediction of precise trajectory for particles, with precise locations and precise energy at every.
The Model of the Atom
1 Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Quantum Theory and the Electronic Structure of.
Atomic Structure the wave nature of light 1 2 3 2 Hz 4 Hz 6 Hz 
4: Introduction to Quantum Physics
Light is a Particle Physics 12.
Introduction to Modern Physics A (mainly) historical perspective on - atomic physics  - nuclear physics - particle physics.
Unit 12: Part 2 Quantum Physics. Overview Quantization: Planck’s Hypothesis Quanta of Light: Photons and the Photoelectric Effect Quantum “Particles”:
Chapter 33 Early Quantum Theory and Models of Atom.
Physics 213 General Physics Lecture Exam 3 Results Average = 141 points.
QUANTUM AND NUCLEAR PHYSICS. Wave Particle Duality In some situations light exhibits properties that are wave-like or particle like. Light does not show.
Quantum Theory Glenn V. Lo Department of Physical Sciences Nicholls State University.
Topic I: Quantum theory Chapter 7 Introduction to Quantum Theory.
Quantum Theory and the Electronic Structure of Atoms Chapter 7.
Chemistry I Chapter 4 Arrangement of Electrons. Electromagnetic Radiation Energy that exhibits wavelike behavior and travels through space Moves at the.
Light Light is a kind of electromagnetic radiation, which is a from of energy that exhibits wavelike behavior as it travels through space. Other forms.
Chapter 6 Electronic Structure of Atoms
Introduction to Quantum Theory for General Chemistry
Atomic Structure the wave nature of light 1 2 3 2 Hz 4 Hz 6 Hz 
Blackbody Radiation PHY361,
Tools of the Laboratory
Atomic Physics & Quantum Effects
Solid Sphere Model or Billiard Ball Model John Dalton
Chapter 27 Early Quantum Theory
Chapter 7: The quantum-mechanical model of the atom
Ch. 13 Electrons in Atoms Ch Models of the Atom
c = speed of light (ms-1, constant)
Presentation transcript:

The mathematics of classical mechanics Newton’s Laws of motion: 1) inertia 2) F = ma 3) action:reaction The motion of particle is represented as a differential equation F = ma = m(dv/dt) = dp/dt Lagrange: Defines the motion of particle in terms of kinetic and potential energy rather than forces. Introduces partial differentials representing each degree of freedom of motion (3D motion) Hamilton: E = K + V — In QM the energy of a particle is determined mathematically by applying the Hamiltonian operator to the wave function representing the particle.

Get Comfortable with units (SI = kg, m, s) Force = Pressure = Energy =

Get Comfortable with units (SI = kg, m, s) Force = m (kg) a (m s -2 ) = kg m s -2 Pressure = F/area = kg m s -2  m 2 = kg m -1 s -2 Energy = F distance = kg m 2 s -2 or PV = kg m -1 s -2 m 3 = kg m 2 s -2 Power = E/t = W (watts) = J s -1 = kg m 2 s -3

classical mechanics vs. quantum mechanics Particle – wave distinction Energy is continuous Deterministic Particle – wave duality uncertainty principle Energy is quantized

Light (emr) – James C. Maxwell (1831 – 1879) CM: 1) emr is a wave form of energy 2) travels through ‘ether’ 3) E is continuous 4) wave amplitude = intensity QM: 1) Photons of light (Relativity ‘removed’ ether) 2) Energy is quantized: E = h 3) Intensity = # photons                                       rays x rays UV IR  waves radio

CLASSICAL MECHANICS failures Atomic structure and spectra: Predicts collapse of electrons into nucleus of atoms No explanation for spectrum of atom Blackbody Radiation: Predicts a heated body will emit infinite energy The Photoelectric Effect Predicts that ↑intensity of emr should be sufficient to expel e - The Equipartition Theory C P of a substance = ½kT for each degree of freedom C P is independent of temperature

Blackbody Radiation A heated object will emit radiation

 CM  d  = 8  kT/ 4 d CM predicts infinite energy would be emitted by a blackbody!  E/V (energy density J m -3 ) slope = d  d QM  d  = {8  hc/ 5 1/{exp(hc/ kT)-1} d

QM predicts a peak of energy density occurring at higher frequencies (lower ) as T↑. This is what is observed. Total power flux (W m -2 or J s -1 m -2 ) =  T 4  = x W m -2 K -4 max (nm) = 2.90 x 10 6 (nm K) ÷ T (K) Sun 5780 K Fe 1811 K NaCl 1074 K Lava~ 1200 K Human 310 K CMBR 2.73K W bulb 3000K dd

Sun Visible range

The Photoelectric Effect E = h = h o + ½mv 2 Light striking a solid metal surface may result in e - expulsion. This is not the same as the 1 st ionization potential which is for gas phase CM – High intensity, low light should be able to cause e - to be emitted! QM – intensity  # of e - expelled (but 1 photon required for each e - ) Threshold o below which no e - emitted regardless of intensity. E > h o imparts extra speed to emitted e -. minimum E to expel e - Kinetic energy of e - metal work function (eV) Na2.36 K2.9 Cs2.14 Mg3.66 Ca2.87 Mn4.1 Nd3.2 Ag4.6 Sn4.42 Pb4.25

Heat Capacity - Oscillations of a solid CM: C V = 3R (constant for all T) QM: C V = 3R at high T - as T  0; C V  0 Although the equipartition theorem makes very accurate predictions in certain conditions, it becomes inaccurate when quantum effects are significant, such as at low temperatures. When the thermal energy kT is smaller than the quantum energy spacing in a particular degree of freedom, the average energy and heat capacity of this degree of freedom are less than the values predicted by equipartition.quantum effectsdegree of freedom Einstein-Bose condensation

Heat Capacity - Oscillations of a solid CM: C V = 3R (constant for all T) QM: C V = 3R at high T - as T  0; C V  0 where  E kT Although the equipartition theorem makes very accurate predictions in certain conditions, it becomes inaccurate when quantum effects are significant, such as at low temperatures. When the thermal energy kT is smaller than the quantum energy spacing in a particular degree of freedom, the average energy and heat capacity of this degree of freedom are less than the values predicted by equipartition.quantum effectsdegree of freedom Einstein-Bose condensation

CM predicts that the electron should radiate energy as it orbits the Nucleus and thus eventually collapse into the nucleus. Observation obviously counters that outcome. ● Atomic Theory: Dalton (1808) – indivisible sphere Thomson (1890s) raisin pudding Rutherford (1908) nuclear model ● emr  emitted

de Broglie E = h  & E = mc 2 replace particle velocity for c (derive expression for ) mv 2 = hv/ = h/mv h  = hc/ = mc 2 in 1927 Ni crystal observed to diffract e - beam 1 st observation of wave properties of ‘particle’

The Bohr Atom - Postulates Energy is Quantized Atoms in stationary state will not emit radiation An atom absorbs or emits radiation as it changes state The Bohr Atom Orbit has radius such that angular momentum, L = mvr = nħ ● The energy of the orbits are quantized (eq. 9.31) 0.529Å